The effects of delta-9-tetrahydrocannabinol on actin microfilaments

Fluorescence staining with rhodamine phalloidin specific for F-actin was employed to examine the effects of delta-9-tetrahydrocannabinol (THC) on the distribution of microfilaments in kangaroo rat epithelial cells (PtK2) and rabbit aortic endothelial cells (RAE). PtK2 cells were more sensitive to THC treatment than RAE cells. Exposure of PtK2 cells to 10 microM THC for 2 h disrupted the microfilament network. After treatment with 20 microM THC for 2 h there was a loss of cell-to-cell contact between PtK2 cells, and at 30 microM THC, the cells started to detach from the substratum. In contrast, microfilament disorganization but not cell detachment was observed in RAE cells at THC concentrations of 80 and 100 microM. The possible mechanisms which may account for the changes in the microfilament system are discussed.     

The effects of p-mercuribenzenesulfonate on purified spectrin and actin

The compound p-mercuribenzenefulfonate was found to affect the self-association behavior of both spectrin and actin. The reagent brings about the depolymerization of F-actin, as judged from the decrease in the fluorescence of an attached pyrene label, with a second-order rate constant an order of magnitude less than that for the disruption of isolated erythrocyte cytoskeletons. Therefore, it is unlikely that the depolymerization of actin is the rate-determining step in the mercurial-dependent disruption of the erythrocyte cytoskeleton. Low reagent concentrations caused an initial rapid dissociation of spectrin tetramers at a rate comparable with that of cytoskeleton disruption. Prolonged incubation, or higher reagent concentrations, resulted in subsequent aggregation of spectrin. The reagent also prevented the interaction between spectrin and actin, presumably through its depolymerization of actin and its effects on spectrin. The early event in the disruption of isolated erythrocyte cytoskeletons by p-mercuribenzenesulfonate thus appears to be the dissociation of spectrin oligomers. Subsequent depolymerization of actin brought about by the reagent then results in total disruption of the cytoskeleton.     

Effects of chaetoglobosin J on the G-F transformation of actin

It was shown that substoichiometric concentrations of chaetoglobosin J, one of the fungal metabolites belonging to cytochalasins, inhibited the elongation at the barbed end of an actin filament. Stoichiometric concentrations of chaetoglobosin J decreased both the rate and the extent of actin polymerization in the presence of 75 mM KCl, 0.2 mM ATP and 10 mM Tris-HCl buffer at pH 8.0 and 25 degrees C. In contrast, stoichiometric concentrations of cytochalasin D accelerated actin polymerization. Chaetoglobosin J slowly depolymerized F-actin to G-actin until an equilibrium was reached. Analyses by a number of different methods showed the increase of monomer concentration at equilibrium to depend on chaetoglobosin J concentrations. F-actin under the influence of stoichiometric concentrations of chaetoglobosin J only slightly activated the Mg2+-enhanced ATPase activity of myosin at low ionic strength. It is suggested that when the structure of the chaetoglobosin-affected actin filaments is modified, the equilibrium is shifted to the monomer side, and the interaction with myosin is weakened.     

The effects of cytochalasins on actin polymerization and actin ATPase provide insights into the mechanism of polymerization

Substoichiometric concentrations of cytochalasin D inhibited the rate of polymerization of actin in 0.5 mM MgCl2, increased its critical concentration and lowered its steady state viscosity. Stoichiometric concentrations of cytochalasin D in 0.5 mM MgCl2 and even substoichiometric concentrations of cytochalasin D in 30 mM KCl, however, accelerated the rate of actin polymerization, although still lowering the final steady state viscosity. Cytochalasin B, at all concentrations in 0.5 mM MgCl2 or in 30 mM KCl, accelerated the rate of polymerization and lowered the final steady state viscosity. In 0.5 mM MgCl2, cytochalasin D uncoupled the actin ATPase activity from actin polymerization, increasing the ATPase rate by at least 20 times while inhibiting polymerization. Cytochalasin B had a very much lower stimulating effect. Neither cytochalasin D nor B affected the actin ATPase activity in 30 mM KCl. The properties of cytochalasin E were intermediate between those of cytochalasin D and B. Cytochalasin D also stimulated the ATPase activity of monomeric actin in the absence of MgCl2 and KCl and, to a much greater extent, stimulated the ATPase activity of monomeric actin below its critical concentration in 0.5 mM MgCl2. Both above and below its critical concentration and in the presence and absence of cytochalasin D, the initial rate of actin ATPase activity, when little or no polymerization had occurred, was directly proportional to the actin concentration and, therefore, apparently was independent of actin-actin interactions. To rationalize all these data, a working model has been proposed in which the first step of actin polymerization is the conversion of monomeric actin-bound ATP, A . ATP, to monomeric actin-bound ADP and Pi, A* . ADP . Pi, which, like the preferred growing end of an actin filament, can bind cytochalasins.     

The effects of smooth muscle caldesmon on actin filament motility.

The movement of reconstituted thin filaments over an immobilized surface of thiophosphorylated smooth muscle myosin was examined using an in vitro motility assay. Reconstituted thin filaments contained actin, tropomyosin, and either purified chicken gizzard caldesmon or the purified COOH-terminal actin-binding fragment of caldesmon. Control actin-tropomyosin filaments moved at a velocity of 2.3 +/- 0.5 microns/s. Neither intact caldesmon nor the COOH-terminal fragment, when maintained in the monomeric form by treatment with 10 mM dithiothreitol, had any effect on filament velocity; and yet both were potent inhibitors of actin-activated myosin ATPase activity, indicating that caldesmon primarily inhibits myosin binding as reported by Chalovich et al. (Chalovich, J. M., Hemric, M. E., and Velaz, L. (1990) Ann. N. Y. Acad. Sci. 599, 85-99). Inhibition of filament motion was, however, observed under conditions where cross-linking of caldesmon via disulfide bridges was present. To determine if monomeric caldesmon could "tether" actin filaments to the myosin surface by forming an actin-caldesmon-myosin complex as suggested by Chalovich et al., we looked for caldesmon-dependent filament binding and motility under conditions (80 mM KCl) where filament binding to myosin is weak and motility is not normally seen. At caldesmon concentrations > or = 0.26 microM, actin filament binding was increased and filament motion (2.6 +/- 0.6 microns/s) was observed. The enhanced motility seen with intact caldesmon was not observed with the addition of up to 26 microM COOH-terminal fragment. Moreover, a molar excess of the COOH-terminal fragment competitively reversed the enhanced binding seen with intact caldesmon. These results show that tethering of actin filaments to myosin by the formation of an actin-caldesmon-myosin complex enhanced productive acto-myosin interaction without placing a significant mechanical load on the moving filaments.     

Pressure effects on actin self-assembly: interspecific differences in the equilibrium and kinetics of the G to F transformation

Purified skeletal muscle actins from species whose ambient pressures range from 1 to greater than 500 atm were examined for the sensitivity to hydrostatic pressure of the globular (G) to filamentous (F) self-assembly reaction. Both the equilibrium position and the kinetics of self-assembly were affected by pressure. Increased pressure shifted the self-assembly equilibrium toward the monomer (G) state and reduced the rate of F-actin assembly. For most of the actins studied, the perturbation by pressure of F-actin formation decreased with increasing measurement of pressure, indicating that F-actin has a higher compressibility than G-actin. The increase in system volume and compressibility concomitant with the assembly of F-actin can be interpreted as reflections of the major role played by hydrophobic effects in stabilizing F-actin and of the existence of "hard" binding sites, in the terminology of Torgerson et al. [Torgerson, P. M., Drickamer, H. G., & Weber, G. (1979) Biochemistry 18, 3079-3083], in the actin subunits. For actin from the deepest occurring species studied, the teleost fish Coryphaenoides armatus, which occurs to depths of approximately 5000 m (equivalent to 501 atm of pressure), there was no difference in compressibility between G-actin and F-actin; that is, the effect of increasing pressure on self-assembly was linear over the entire pressure range examined, 600 atm. The self-assembly reaction of the actin from C. armatus also differed from that of the other actins examined in that the G to F equilibrium was relatively insensitive to increased pressure; i.e., the volume change (delta V) of assembly was small.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effects of actin on the electron spin resonance of spin-labeled myosin

Myosin and heavy meromyosin have been spin labeled at either the S₁ or S₂ thiol groups, and their interaction with F-actin has been studied by electron spin resonance, both in the absence of substrate and during the hydrolysis of ATP. The spectrum of myosin labeled at either group indicates strong immobilization of the label. In the absence of substrate, actin added to S₁-labeled myosin slightly increases the separation of the outer spectral peaks, indicating a decrease in the mobility of the spin label. Actin also reduces the microwave power required to saturate the esr signal of S₁-labeled myosin or heavy meromyosin. The latter phenomenon is a more sensitive measure of the actin-myosin interaction than the spectral change seen in the absence of saturation. This suggests that saturation measurements may provide a more sensitive method of detecting changes in the environment of slowly tumbling nitroxide radicals than spectral measurements carried out in the absence of saturation. The decrease in the amplitude of the spectrum on adding actin at saturating microwave power was used to determine the stoichiometry of the interaction between actin and heavy meromyosin. This decrease is maximal when 2 moles of actin monomer are added per mole of heavy meromyosin and is reversed when actin and myosin are dissociated by ATP. During the steady state hydrolysis of ATP, actin had no detectable effect on the spectrum of S₁-labeled myosin. It can be concluded that spin labels bound to the S₁ groups are in a region of the myosin molecule that is affected by the interaction with actin. Actin does not affect the rate at which the bound spin label is reduced by dithiothreitol nor does the spin labeling of S₁ groups affect the activation by actin of the ATPase activity of myosin. These findings suggest that the most likely mechanism by which actin alters the mobility of labels on S₁ groups involves a change in the conformation of myosin. If a spin label is bound to the S₂ thiol groups rather than the S₁ groups, then actin has no detectable effect on the spectrum either in the presence or absence of ATP.     

A mutation in actin associated with neoplastic transformation

A new protein was recognized in a chemically transformed human fibroblast cell line when its proteins labeled with [35S]methionine were compared with those from normal human fibroblasts by two-dimensional gel electrophoresis. The new protein was found in the Triton-insoluble cytoskeletal fraction as well as in the Triton-soluble fraction, and it migrated very closely to beta- and gamma-actins on the gels. This new protein was identified as a variant form of actin by its reaction with antiactin antibody and its tryptic peptide pattern, which was identical to actin. mRNA coding for the variant actin was detected only in this particular transformed line. The size and cross- hybridizability with Dictyostelium actin cDNA of mRNA coding for the variant actin and complete amino acid sequence of the variant actin indicate that the new variant actin is the product of a mutated beta-actin gene. Only a single amino acid (glycine) at position 244 was replaced by aspartic acid. This substitution corresponds to a GC----AT transition, a point mutation. On the other hand, a highly malignant cell variant was isolated from the transformed line. The mutated beta-actin was further altered in this highly malignant subclone: it showed a more negative charge, rapid synthetic rate, and a short half-life in the cells. Incorporation into the cytoskeleton was significantly reduced in the mutated beta-actin. A hypothesis on the relationship between a mutation in the actin gene and oncogenic transformation was proposed.     

Advances in Rho-dependent actin regulation and oncogenic transformation.

Cellular movement is central to invasion. The Rho family of small GTPases co-ordinate the cytoskeletal and adhesion modelling within cells that is crucial for normal migratory responses. Consequently, Rho proteins, and their regulators and effectors, are targets for subversion during oncogenic transformation and tumour development. Recent findings have thrown light on how actin regulators may be linked to oncogenesis and the development of cancer.     

Allele-specific effects of thoracic aortic aneurysm and dissection alpha-smooth muscle actin mutations on actin function

Twenty-two missense mutations in ACTA2, which encodes α-smooth muscle actin, have been identified to cause thoracic aortic aneurysm and dissection. Limited access to diseased tissue, the presence of multiple unresolvable actin isoforms in the cell, and lack of an animal model have prevented analysis of the biochemical mechanisms underlying this pathology. We have utilized actin from the yeast Saccharomyces cerevisiae, 86% identical to human α-smooth muscle actin, as a model. Two of the known human mutations, N115T and R116Q, were engineered into yeast actin, and their effect on actin function in vivo and in vitro was investigated. Both mutants exhibited reduced ability to grow under a variety of stress conditions, which hampered N115T cells more than R116Q cells. Both strains exhibited abnormal mitochondrial morphology indicative of a faulty actin cytoskeleton. In vitro, the mutant actins exhibited altered thermostability and nucleotide exchange rates, indicating effects of the mutations on monomer conformation, with R116Q the most severely affected. N115T demonstrated a biphasic elongation phase during polymerization, whereas R116Q demonstrated a markedly extended nucleation phase. Allele-specific effects were also seen on critical concentration, rate of depolymerization, and filament treadmilling. R116Q filaments were hypersensitive to severing by the actin-binding protein cofilin. In contrast, N115T filaments were hyposensitive to cofilin despite nearly normal binding affinities of actin for cofilin. The mutant-specific effects on actin behavior suggest that individual mechanisms may contribute to thoracic aortic aneurysm and dissection.     

Nucleotide effects on the structure and dynamics of actin

Adenosine 5'-triphosphate or ATP is the primary energy source within the cell, releasing its energy via hydrolysis into adenosine 5'-diphosphate or ADP. Actin is an important ATPase involved in many aspects of cellular function, and the binding and hydrolysis of ATP regulates its polymerization into actin filaments as well as its interaction with a host of actin-associated proteins. Here we study the dynamics of monomeric actin in ATP, ADP-Pi, and ADP states via molecular dynamics simulations. As observed in some crystal structures we see that the DNase-I loop is an alpha-helix in the ADP state but forms an unstructured coil domain in the ADP-Pi and ATP states. We also find that this secondary structure change is reversible, and by mimicking nucleotide exchange we can observe the transition between the helical and coil states. Apart from the DNase-I loop, we also see several key structural differences in the nucleotide binding cleft as well as in the hydrophobic cleft between subdomains 1 and 3 where WH2-containing proteins have been shown to interact. These differences provide a structural basis for understanding the observed differences between the various nucleotide states of actin and provide some insight into how ATP regulates the interaction of actin with itself and other proteins.     

The role of actin in temperature-dependent gel-sol transformation of extracts of Ehrlich ascites tumor cells

Ehrlich ascites tumor cell extracts form a gel when warmed to 25 degrees C at pH 7.0 in sucrose solution, and the gel rapidly becomes a sol when cooled to 0 degrees C. This gel-sol transformation was studied quantitatively by determining the volume or the total protein of pellets of gel obtained by low-speed centrifugation. The gelation depended on nucleotide triphosphates, Mg2+, KCl, and a reducing agent. Gelation was inhibited reversibly by 0.5 microM free Ca2+, and 25--50 ng/ml of either cytochalasin B or D, but it was not affected by 10 mM colchicine. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis demonstrated that the gel was composed of six major proteins with mol wt greater than 300,000, 270,000, 89,000, 51,000, 48,000, and 42,000 daltons. The last component was identified as cell actin because it had the same molecular weight as muscle actin and bound with muscle myosin and tropomyosin. The role of actin in gelation was studied by use of actin-inhibitors. Gelation was inhibited by a chemically modified subfragment-1 of myosin, which binds with F-actin even in the presence of ATP, and by bovine pancreatic DNase I, which tightly binds with G-actin. Muscle G-actin neutralized the inhibitory effect of DNase I when added at an equimolar ratio to the latter, and it also restored gelation after its inhibition by DNase I. These findings suggest that gelation depends on actin. However, the extracts showed temperature-dependent, cytochalasin-sensitive, and Ca2+-regulated gelation as did the original extracts when the cell actin in the extracts was replaced by muscle actin, suggesting that components other than cell actin might be responsible for these characteristics of the gelation.     

The effects of pressure on yeast cytochrome c peroxidase

The effects of pressure on cytochrome c peroxidase [CcP(FeIII)], its cyano derivative (CcP X CN) and its enzyme-substrate complex (ES) have been studied. The effects of pressure on the binding of the substrate analog porphyrin cytochrome c (porphyrin c) to CcP X CN and ES have also been studied. High pressure causes CcP(FeIII) to undergo a high-spin to low-spin transition but has no detectable effect on either CcP X CN, which is already low spin, or on ES. The low-spin CcP(FeIII) structure at pressure is similar to the low-spin form at low temperature and the low-spin form of horseradish peroxidase at high pressure. delta V degree associated with the spin equilibrium is about 30 ml/mol and is independent of temperature. delta G degree is small, 4.7 kJ/mol at 0 degree C, while delta H degree is 14.2 kJ/mol at 1 bar (100 kPa). Pressure has no detectable effect on the binding equilibria of mixtures of CcP X CN plus porphyrin c or ES plus porphyrin c. This indicates that the interaction of CcP and porphyrin c results in little or no volume change; the same is true in the case of cytochrome c oxidase and porphyrin c.     

Protein osmotic pressure modulates actin filament length distribution

1.

The changes of the macromolecular osmotic pressure associated with F-actin solutions are related to the changes of the free energy of the free actin monomers.

2.

By making use of the model of Biron et al. [2006. Inter-filament attractions narrow the length distribution of actin filaments. Europhys. Lett. 73, 464-470], the changes of the free energy of the free actin monomers are related to the changes of the length distribution of the actin filaments.

On these bases, we propose that the length distribution of the actin filaments is regulated by (a) the free energy of hydrolysis of ATP and (b) the macromolecular osmotic pressure.

a.

While the free energy of hydrolysis of ATP tends to zero, the length distribution of the actin filaments shifts from an exponential curve to a straight line parallel to the abscissa axis (i.e. the concentration of the actin filaments becomes independent of their length). In the mean time, the total energy of the actin filaments reaches a minimum.

b.

With the increase of the macromolecular osmotic pressure the free energy of the actin monomers increases and a break is introduced in the curve that describes the length distribution of the actin filaments; the break is located at the mean length of the filaments.